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The Pluto Experiment at Doris (Desy) And THE PLUTO EXPERIMENT AT DORIS (DESY) AND THE DISCOVERY OF THE GLUON. (A RECOLLECTION). Bruno R. Stella1 Department of Physics of Roma Tre University and INFN; Rome, Italy Hans-Jürgen Meyer2 formerly at Department of Physics, Siegen University; Siegen, Germany (to be submitted to The European Physical Journal H) Abstract. With the aim of determining the contribution of the PLUTO experiment at the DORIS e+e- storage ring to the discovery of the gluon, as members of this former collaboration we have reconsidered all the scientific material produced by PLUTO in 1978 and the first half of 1979. It is clear that the experiment demonstrated the main decay of the Y(9.46 GeV) resonance to be mediated by 3 gluons, by providing evidence for the agreement of this hypothesis with average values and differential distributions of all possible experimental variables and by excluding all other possible alternative models. Moreover PLUTO measured in June 1979 the matrix element of the 3-gluon decay to be quantitatively as expected by QCD (even after hadronization) and, having checked the possibility to correctly trace the gluons’ directions, demonstrated the spin 1 nature of the gluon by excluding spin 0 and spin ½. The hadronization of the gluon like a quark jet, hypothesized in the 3-gluon jet Monte Carlo simulation, was compatible with the topological data at this energy and was shown to -1 be an approximation at 10% level for the multiplicity (≈<p||> ); the right expected gluon fragmentation was needed for the inclusive distributions; this was the first experimental study of (identified) gluon jets. In the following measurements at the PETRA storage ring, these results were confirmed by PLUTO and by three contemporaneous experiments by evidencing at higher energies the gluon radiation (“bremsstrahlung”), the softer one, by jet broadening, and the hard one, by the emission of (now clearly visible) gluon jets by quarks. The gluon’s spin 1 particle nature was also confirmed. The PLUTO results on Y decays had been confirmed both by contemporaneous experiments at DORIS (partially) and later (also partially) were confirmed by more sophisticated detectors. 1 Introduction Quantum Chromodynamics (QCD, the theory of strong interactions) and the gluon, the messenger of the strong (“color”) force, were proposed (after an early paper by Gell-Mann in 1962 [1]) in the years 1970-1980 [2], in parallel and after the quark parton model was stabilized. A 1 e-mail: [email protected] 2 e-mail: [email protected] 1 laboratory for studying QCD and gluons was proposed to be the next heavy narrow hadronic resonance [3-6]. In 1977 the Y(9.46 GeV) resonance was discovered at Fermilab [7] and its very narrow width (≈50 keV) was found at DORIS (3-10 GeV e+e- storage ring at DESY) by the experiments PLUTO and DASP2 in May 1978 [8]. The first evidence for the abundant decay of Y into 3 gluons was reported by the PLUTO Collaboration, at Schools and Conferences in Summer 1978 [9-17], as well as in publications [18-20]. Further presentations followed at Winter [21,22] and Spring [23-25] schools and meetings, and the cross sections were given in the thesis [26]. In June 1979 at the Geneva International Conference [27] the evidence for the Y decay into 3 gluons (with the partonic matrix element) was presented by PLUTO [28, mentioned also in 29,30] and the first evidence at PETRA (the new 10-48 GeV e+e- storage ring at DESY) for quark jet broadening by gluon radiation was shown by TASSO [30] and also with more results by PLUTO [31]. At the following Lepton-Photon Symposium at FermiLab [32] PLUTO showed the step due to the production of the new quark b and confirmed the jet broadening [33] and the 3-gluon interpretation of the Y decay [34]. At this conference the evidence for three jet events (interpreted as gluon radiation by a pair) was shown by the TASSO, PLUTO, MARK-J and JADE experiments at PETRA [36-41] again confirming the existence of gluon jets now at a factor three larger energies. As members of the PLUTO Collaboration, after more than thirty years we think it timely and worthwhile to recollect and recall in this article, and for a wider public, what PLUTO did in relation to the gluon discovery in the years 1978 and first half of 1979 and the confirmations obtained both at DORIS and at PETRA. In chapter 2 we briefly summarize the related physics highlights preceeding the PLUTO experiment at DORIS; in chapter 3 we sketch the PLUTO detector and the properties of the DORIS and PETRA storage rings, with a brief history of the machines and the detector; in chapter 4 we sketch the simulations of the physical processes. In the main chapter 5 we recollect the elements for the discovery of the Y→3-gluon decay: the Y resonance; inclusive dynamics; geometry (topology); exclusion of alternative models; exclusive 3-gluon dynamics and gluon hadronization (the first study of gluon jets). All with the aim to single out the sufficient and the necessary conditions to demonstrate the validity of the 3-gluon hypothesis (QCD). In chapter 6 we cover the confirmations found at DORIS, especially by a more sophisticated detector (ARGUS), as well by CLEO at the CESR storage ring, Cornell, USA, the jet broadening found at PETRA and the most important confirmation for the gluon: the discovery of gluon bremsstrahlung. Finally we give a summary and draw the conclusions in chapter 7. 2 Prologue: The related physics in the years 1974-1978 The pointlike fractionally charged constituents of the elementary particles (partons or quarks) were hypothesized and found in the years 1964-1974. The last step, the number of quarks, was + - + - + - demonstrated experimentally by measuring R, the ratio σ(e e hadrons) / σ(e e μ μ ), a measurement of the sum of the square of the quark charges divided by the square of the muon’s charge. A new quantum number (“color”) was needed to justify the high R value measured at e+e- colliders [42]. In 1974 a very narrow resonance was discovered [43], the J/ψ(3.1 GeV), recognised to be the ground state of a new resonance, of the “charm” quark, “charmonium” ( ). In 1975 excited states were found, starting the field of charmonium spectroscopy [44]. Using the measured J/ψ + - + - cross section and the J/ψe e , μ μ branching ratios, in non-relativistic potential models for quark binding, the charm quark was shown to have a charge ⅔ of the proton charge. The presence and 2 charge of the new quark was also seen in e+e- annihilations as a step in R outside the resonance region. In 1975 Appelquist and Politzer [3] proposed (in analogy with the orthopositronium decay into 3 photons calculated with QED by Ore and Powell [45]) that a narrow resonance found in e+e- annihilation (with the quantum numbers of the photon, as orthopositronium decaying into 3 γ’s) should decay into 3 gluons, the supposed exchange particle of the strong interactions (with the same quantum numbers of the photon, plus “color”: QCD is the name of the resulting theory). In the same year at SPEAR [46] at 7.4 Gev the first “jets” of particles were seen in e+e- → annihilations, a mechanism proposed [47-53] for the hadronization of quarks and gluons. (This means that a jet of 3.7 GeV or more is visible sometimes by the naked eye as a separate cluster of particles of limited transverse momentum with respect to its mean longitudinal momentum). A new heavy lepton, the tau (τ), was also found in 1975 *54+ as a third charged lepton (after the electron and the muon). The τ, being heavy enough, can decay also into hadrons. Its existence implied the existence of a new heavy quark doublet (“beauty” and “truth” or “bottom” and “top”) paired with it and the tau neutrino (according to the hypotheses of Glashow, Iliopulos and Maiani and of Kobajashi and Maskawa [55]). The properties of the possible ground state were predicted in detail by Eichten and Gottfried in 1977 [56]. In 1976, Ellis, Gaillard and Ross [50] proposed that high energy quarks should radiate gluons (a 1— neutral massless colored particle) very much as in QED the electrons radiate photons. The pairs produced in e+e- annihilations could radiate gluons (gluon bremsstrahlung) and those gluons could manifest themselves as a cascade of quarks and gluons and finally ordinary hadrons: jets again [50-52]. In 1976 the charmed mesons D and D* were discovered as bound states of a “light (u,d,s)” quark and the new charm quark [44]. In 1977 a Y(9.5 GeV) heavy resonance was discovered in an experiment at Fermilab of a proton beam striking a nuclear target [7], relatively narrow (±200 MeV, compatible with the resolution of the experiment) and seen in the μ+μ- decay. Koller and Walsh [4] and in 1978-79 together with Krasemann, Zerwas and Kramer [6] and Fritzsch and Streng [5] proposed a test of QCD by looking for gluon jets in the decay of a heavy quark-antiquark bound state produced in e+e- annihilations and calculated the gluon or jet (the forward product of its hadronization) angular distributions, estimating also multiplicities and momentum distributions of hadrons in a 3 gluons 3 jets final state. When, at DESY, the Y(9.46) was confirmed by PLUTO to be an extremely narrow state [8,76] but with abundant hadronic decays, it was clear that it was not decaying as a ‘normal’ hadronic resonance: it was a possible candidate for the proposed 3-gluon decay.
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